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Given an inner product space , the orthogonal group of is the subgroup of the general linear group which leaves invariant the inner product.
Given an element of we say it preserves the inner product if for all .
If and preserve the inner product on , then so do and .
We thus see that we have a group.
The orthogonal group is the subgroup of consisting of those elements that preserve the inner product.
(… more detail …)
When the base field is , or (the last being a skewfield, but this is ok), and the vector space is finite-dimensional then we can put the structure of a finite-dimensional manifold on . We shall denote the group in this case by where , and we take the ‘standard’ inner products on these spaces.
A relatively easy way to see that is a manifold is that it is a smooth affine variety in Euclidean space, but this requires some machinery. We can however construct explicit charts for as a real manifold.
One can use the algebra structure on matrices over the base field (or base division ring) of to define charts which are different to the charts one gets via the exponential map.
For Define the sets
and
Here is a vector space, and will turn out to be the tangent space to at .
There is an isomorphism .
The map is defined as
the latter equality using that . We need to check that this is indeed a map to and that it is an isomorphism.
Since
if we show that we are done. Let , which is again in . Then
(tbc…)
Euclidean space with the standard inner product has as orthogonal group the standard orthogonal group .
The finite-dimensional Hilbert space with the standard inner product has as orthogonal group , the unitary group
The space , for the quaternions, has an inner product … such that the corresponding orthogonal group is the compact symplectic group .
(…Examples of indefinite signature go here…)
Last revised on August 14, 2013 at 13:05:31. See the history of this page for a list of all contributions to it.